RF inductors - SMD

RF (Radio Frequency) inductors in SMD (Surface Mount Device) form are specialized components used in high-frequency electronic circuits and applications. SMD RF inductors are designed to be mounted directly onto the surface of a circuit board, offering advantages such as space-saving, easy assembly, and compatibility with automated manufacturing processes.
RF inductors are specifically optimized for operation at radio frequency ranges, typically from a few megahertz (MHz) up to several gigahertz (GHz). They are commonly used in RF applications, including RF filters, oscillators, RF amplifiers, impedance matching networks, and wireless communication systems.
SMD RF inductors feature a compact design and are constructed similarly to other inductors. They consist of a coil wound on a core material, but with specific considerations for high-frequency performance and minimizing parasitic effects. These parasitic effects include self-capacitance, series resistance, and interwinding capacitance, which can impact the inductor's performance at high frequencies.
The core materials used in SMD RF inductors are carefully chosen to provide high magnetic permeability, low losses, and stable performance across the desired frequency range. Common core materials for RF inductors include ceramic materials, ferrite, and powdered iron.
SMD RF inductors come in various package sizes and shapes, denoted by standardized codes such as 0402, 0603, or 0805, indicating their dimensions in terms of length and width. This allows for easy integration into surface mount technology and efficient assembly onto circuit boards.
When selecting SMD RF inductors, critical parameters to consider include inductance value, quality factor (Q factor), self-resonant frequency (SRF), and maximum current handling capability. The inductance value determines the component's ability to store energy in its magnetic field, while the Q factor represents its efficiency and ability to maintain high-quality performance. The SRF indicates the frequency at which the inductor starts to exhibit resonance due to its parasitic capacitance. Maximum current handling capability is crucial for ensuring the inductor can withstand the power demands of the RF circuit.
SMD RF inductors are chosen based on specific circuit requirements, such as the desired operating frequency, impedance matching, bandwidth, and available board space. They are essential components in RF systems, contributing to impedance control, filtering, and energy storage functions necessary for reliable and efficient RF signal processing and wireless communication.
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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
BSCH000603035N6S00


RF Inductors - SMD 5.6nH RDC=0.36Ohms 260mA
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Pulse 14259
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AUD 0.0152
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 0.6 mm x 0.3 mm x 0.3 mmShielded5.6 nH0.3 nH 360 mOhms260 mA- 55 C+ 125 C44.6 GHzStandard0.6 mm0.3 mm0.3 mm Ceramic BSCHReel , Cut Tape
LQP03TN2N0BZ2D


RF Inductors - SMD
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Murata 14259
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AUD 0.0221
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Thin Film0201 (0603 METRIC)Unshielded2 nH0.1 nH600 mA150 mOhms-- 55 C+ 125 C1412.5 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
MLG0603P2N7CTD25


RF Inductors - SMD IND 0201 2.7nH Hi-Q AEC Q200 RF IND
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TDK 14249
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AUD 0.044
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Multilayer0201 (0603 METRIC)Unshielded2.7 nH0.2 nH500 mA200 mOhms-- 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLG - PReel , Cut Tape
MLF1005G1R8KT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 30mA, 1.8?H, 1.05ohm
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TDK 14248
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AUD 0.1535
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Multilayer0402 (1005 METRIC)Shielded1.8 uH10 %30 mA1.05 Ohms-- 55 C+ 125 C30180 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
MLG0603S62NJTD25


RF Inductors - SMD IND 0201 62nH StdQ AEC Q200 RF IND
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TDK 14239
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AUD 0.0565
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Multilayer0201 (0603 METRIC)Unshielded62 nH5 %50 mA3.3 Ohms-- 55 C+ 125 C51.3 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQP02HQ1N6B02E


RF Inductors - SMD
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Murata 14236
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AUD 0.0959
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Thin Film01005 (0402 METRIC)Unshielded1.6 nH0.1 nH700 mA80 mOhms-- 55 C+ 125 C1410.7 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW15AN43NG8ZD


RF Inductors - SMD 43 NH 2%
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Murata 14230
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AUD 0.1535
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Wirewound0402 (1005 METRIC)Unshielded43 nH2 %515 mA516 mOhms-- 55 C+ 125 C303.4 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
Hot LQP03HQ9N1H02D


RF Inductors - SMD 9.1 NH 3% NH
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Murata 14220
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AUD 0.0358
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Thin Film0201 (0603 METRIC)Unshielded9.1 nH3 %300 mA400 mOhms-- 55 C+ 125 C204.5 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
MLG0603SR15JT000


RF Inductors - SMD IND 0201 150nH StdQ SMD RF IND
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TDK 14214
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AUD 0.0417
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Multilayer0201 (0603 METRIC)Unshielded150 nH5 %50 mA8 Ohms-- 55 C+ 125 C5770 MHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
MLG0603P51NJT000


RF Inductors - SMD IND 0201 51nH Hi-Q SMD RF IND
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TDK 14210
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AUD 0.0294
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Multilayer0201 (0603 METRIC)Unshielded51 nH5 %100 mA3.5 Ohms-- 55 C+ 125 C101.9 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
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